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/**************************************************************************/
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/* basis.cpp */
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/**************************************************************************/
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# include "basis.h"
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# include "core/math/math_funcs.h"
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# include "core/string/ustring.h"
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# define cofac(row1, col1, row2, col2) \
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( rows [ row1 ] [ col1 ] * rows [ row2 ] [ col2 ] - rows [ row1 ] [ col2 ] * rows [ row2 ] [ col1 ] )
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void Basis : : invert ( ) {
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real_t co [ 3 ] = {
cofac ( 1 , 1 , 2 , 2 ) , cofac ( 1 , 2 , 2 , 0 ) , cofac ( 1 , 0 , 2 , 1 )
} ;
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real_t det = rows [ 0 ] [ 0 ] * co [ 0 ] +
rows [ 0 ] [ 1 ] * co [ 1 ] +
rows [ 0 ] [ 2 ] * co [ 2 ] ;
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# ifdef MATH_CHECKS
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ERR_FAIL_COND ( det = = 0 ) ;
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# endif
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real_t s = 1.0f / det ;
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set ( co [ 0 ] * s , cofac ( 0 , 2 , 2 , 1 ) * s , cofac ( 0 , 1 , 1 , 2 ) * s ,
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co [ 1 ] * s , cofac ( 0 , 0 , 2 , 2 ) * s , cofac ( 0 , 2 , 1 , 0 ) * s ,
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co [ 2 ] * s , cofac ( 0 , 1 , 2 , 0 ) * s , cofac ( 0 , 0 , 1 , 1 ) * s ) ;
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}
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void Basis : : orthonormalize ( ) {
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// Gram-Schmidt Process
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Vector3 x = get_column ( 0 ) ;
Vector3 y = get_column ( 1 ) ;
Vector3 z = get_column ( 2 ) ;
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x . normalize ( ) ;
y = ( y - x * ( x . dot ( y ) ) ) ;
y . normalize ( ) ;
z = ( z - x * ( x . dot ( z ) ) - y * ( y . dot ( z ) ) ) ;
z . normalize ( ) ;
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set_column ( 0 , x ) ;
set_column ( 1 , y ) ;
set_column ( 2 , z ) ;
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}
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Basis Basis : : orthonormalized ( ) const {
Basis c = * this ;
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c . orthonormalize ( ) ;
return c ;
}
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void Basis : : orthogonalize ( ) {
Vector3 scl = get_scale ( ) ;
orthonormalize ( ) ;
scale_local ( scl ) ;
}
Basis Basis : : orthogonalized ( ) const {
Basis c = * this ;
c . orthogonalize ( ) ;
return c ;
}
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// Returns true if the basis vectors are orthogonal (perpendicular), so it has no skew or shear, and can be decomposed into rotation and scale.
// See https://en.wikipedia.org/wiki/Orthogonal_basis
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bool Basis : : is_orthogonal ( ) const {
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const Vector3 x = get_column ( 0 ) ;
const Vector3 y = get_column ( 1 ) ;
const Vector3 z = get_column ( 2 ) ;
return Math : : is_zero_approx ( x . dot ( y ) ) & & Math : : is_zero_approx ( x . dot ( z ) ) & & Math : : is_zero_approx ( y . dot ( z ) ) ;
}
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// Returns true if the basis vectors are orthonormal (orthogonal and normalized), so it has no scale, skew, or shear.
// See https://en.wikipedia.org/wiki/Orthonormal_basis
bool Basis : : is_orthonormal ( ) const {
const Vector3 x = get_column ( 0 ) ;
const Vector3 y = get_column ( 1 ) ;
const Vector3 z = get_column ( 2 ) ;
return Math : : is_equal_approx ( x . length_squared ( ) , 1 ) & & Math : : is_equal_approx ( y . length_squared ( ) , 1 ) & & Math : : is_equal_approx ( z . length_squared ( ) , 1 ) & & Math : : is_zero_approx ( x . dot ( y ) ) & & Math : : is_zero_approx ( x . dot ( z ) ) & & Math : : is_zero_approx ( y . dot ( z ) ) ;
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}
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// Returns true if the basis is conformal (orthogonal, uniform scale, preserves angles and distance ratios).
// See https://en.wikipedia.org/wiki/Conformal_linear_transformation
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bool Basis : : is_conformal ( ) const {
const Vector3 x = get_column ( 0 ) ;
const Vector3 y = get_column ( 1 ) ;
const Vector3 z = get_column ( 2 ) ;
const real_t x_len_sq = x . length_squared ( ) ;
return Math : : is_equal_approx ( x_len_sq , y . length_squared ( ) ) & & Math : : is_equal_approx ( x_len_sq , z . length_squared ( ) ) & & Math : : is_zero_approx ( x . dot ( y ) ) & & Math : : is_zero_approx ( x . dot ( z ) ) & & Math : : is_zero_approx ( y . dot ( z ) ) ;
}
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// Returns true if the basis only has diagonal elements, so it may only have scale or flip, but no rotation, skew, or shear.
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bool Basis : : is_diagonal ( ) const {
return (
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Math : : is_zero_approx ( rows [ 0 ] [ 1 ] ) & & Math : : is_zero_approx ( rows [ 0 ] [ 2 ] ) & &
Math : : is_zero_approx ( rows [ 1 ] [ 0 ] ) & & Math : : is_zero_approx ( rows [ 1 ] [ 2 ] ) & &
Math : : is_zero_approx ( rows [ 2 ] [ 0 ] ) & & Math : : is_zero_approx ( rows [ 2 ] [ 1 ] ) ) ;
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}
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// Returns true if the basis is a pure rotation matrix, so it has no scale, skew, shear, or flip.
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bool Basis : : is_rotation ( ) const {
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return is_conformal ( ) & & Math : : is_equal_approx ( determinant ( ) , 1 , ( real_t ) UNIT_EPSILON ) ;
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}
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# ifdef MATH_CHECKS
// This method is only used once, in diagonalize. If it's desired elsewhere, feel free to remove the #ifdef.
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bool Basis : : is_symmetric ( ) const {
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if ( ! Math : : is_equal_approx ( rows [ 0 ] [ 1 ] , rows [ 1 ] [ 0 ] ) ) {
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return false ;
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}
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if ( ! Math : : is_equal_approx ( rows [ 0 ] [ 2 ] , rows [ 2 ] [ 0 ] ) ) {
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return false ;
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}
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if ( ! Math : : is_equal_approx ( rows [ 1 ] [ 2 ] , rows [ 2 ] [ 1 ] ) ) {
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return false ;
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}
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return true ;
}
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# endif
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Basis Basis : : diagonalize ( ) {
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// NOTE: only implemented for symmetric matrices
// with the Jacobi iterative method
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# ifdef MATH_CHECKS
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ERR_FAIL_COND_V ( ! is_symmetric ( ) , Basis ( ) ) ;
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# endif
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const int ite_max = 1024 ;
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real_t off_matrix_norm_2 = rows [ 0 ] [ 1 ] * rows [ 0 ] [ 1 ] + rows [ 0 ] [ 2 ] * rows [ 0 ] [ 2 ] + rows [ 1 ] [ 2 ] * rows [ 1 ] [ 2 ] ;
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int ite = 0 ;
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Basis acc_rot ;
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while ( off_matrix_norm_2 > ( real_t ) CMP_EPSILON2 & & ite + + < ite_max ) {
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real_t el01_2 = rows [ 0 ] [ 1 ] * rows [ 0 ] [ 1 ] ;
real_t el02_2 = rows [ 0 ] [ 2 ] * rows [ 0 ] [ 2 ] ;
real_t el12_2 = rows [ 1 ] [ 2 ] * rows [ 1 ] [ 2 ] ;
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// Find the pivot element
int i , j ;
if ( el01_2 > el02_2 ) {
if ( el12_2 > el01_2 ) {
i = 1 ;
j = 2 ;
} else {
i = 0 ;
j = 1 ;
}
} else {
if ( el12_2 > el02_2 ) {
i = 1 ;
j = 2 ;
} else {
i = 0 ;
j = 2 ;
}
}
// Compute the rotation angle
real_t angle ;
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if ( Math : : is_equal_approx ( rows [ j ] [ j ] , rows [ i ] [ i ] ) ) {
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angle = Math_PI / 4 ;
} else {
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angle = 0.5f * Math : : atan ( 2 * rows [ i ] [ j ] / ( rows [ j ] [ j ] - rows [ i ] [ i ] ) ) ;
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}
// Compute the rotation matrix
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Basis rot ;
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rot . rows [ i ] [ i ] = rot . rows [ j ] [ j ] = Math : : cos ( angle ) ;
rot . rows [ i ] [ j ] = - ( rot . rows [ j ] [ i ] = Math : : sin ( angle ) ) ;
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// Update the off matrix norm
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off_matrix_norm_2 - = rows [ i ] [ j ] * rows [ i ] [ j ] ;
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// Apply the rotation
* this = rot * * this * rot . transposed ( ) ;
acc_rot = rot * acc_rot ;
}
return acc_rot ;
}
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Basis Basis : : inverse ( ) const {
Basis inv = * this ;
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inv . invert ( ) ;
return inv ;
}
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void Basis : : transpose ( ) {
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SWAP ( rows [ 0 ] [ 1 ] , rows [ 1 ] [ 0 ] ) ;
SWAP ( rows [ 0 ] [ 2 ] , rows [ 2 ] [ 0 ] ) ;
SWAP ( rows [ 1 ] [ 2 ] , rows [ 2 ] [ 1 ] ) ;
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}
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Basis Basis : : transposed ( ) const {
Basis tr = * this ;
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tr . transpose ( ) ;
return tr ;
}
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Basis Basis : : from_scale ( const Vector3 & p_scale ) {
return Basis ( p_scale . x , 0 , 0 , 0 , p_scale . y , 0 , 0 , 0 , p_scale . z ) ;
}
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// Multiplies the matrix from left by the scaling matrix: M -> S.M
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// See the comment for Basis::rotated for further explanation.
void Basis : : scale ( const Vector3 & p_scale ) {
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rows [ 0 ] [ 0 ] * = p_scale . x ;
rows [ 0 ] [ 1 ] * = p_scale . x ;
rows [ 0 ] [ 2 ] * = p_scale . x ;
rows [ 1 ] [ 0 ] * = p_scale . y ;
rows [ 1 ] [ 1 ] * = p_scale . y ;
rows [ 1 ] [ 2 ] * = p_scale . y ;
rows [ 2 ] [ 0 ] * = p_scale . z ;
rows [ 2 ] [ 1 ] * = p_scale . z ;
rows [ 2 ] [ 2 ] * = p_scale . z ;
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}
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Basis Basis : : scaled ( const Vector3 & p_scale ) const {
Basis m = * this ;
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m . scale ( p_scale ) ;
return m ;
}
Restore the behavior of Spatial rotations recently changed in c1153f5.
That change was borne out of a confusion regarding the meaning of "local" in #14569.
Affine transformations in Spatial simply correspond to affine operations of its Transform. Such operations take place in a coordinate system that is defined by the parent Spatial. When there is no parent, they correspond to operations in the global coordinate system.
This coordinate system, which is relative to the parent, has been referred to as the local coordinate system in the docs so far, but this sloppy language has apparently confused some users, making them think that the local coordinate system refers to the one whose axes are "painted" on the Spatial node itself.
To avoid such conceptual conflations and misunderstandings in the future, the parent-relative local system is now referred to as "parent-local", and the object-relative local system is called "object-local" in the docs.
This commit adds the functionality "requested" in #14569, not by changing how rotate/scale/translate works, but by adding new rotate_object_local, scale_object_local and translate_object_local functions. Also, for completeness, there is now global_scale.
This commit also updates another part of the docs regarding the rotation property of Spatial, which also leads to confusion among some users.
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void Basis : : scale_local ( const Vector3 & p_scale ) {
// performs a scaling in object-local coordinate system:
// M -> (M.S.Minv).M = M.S.
* this = scaled_local ( p_scale ) ;
}
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void Basis : : scale_orthogonal ( const Vector3 & p_scale ) {
* this = scaled_orthogonal ( p_scale ) ;
}
Basis Basis : : scaled_orthogonal ( const Vector3 & p_scale ) const {
Basis m = * this ;
Vector3 s = Vector3 ( - 1 , - 1 , - 1 ) + p_scale ;
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bool sign = signbit ( s . x + s . y + s . z ) ;
Basis b = m . orthonormalized ( ) ;
s = b . xform_inv ( s ) ;
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Vector3 dots ;
for ( int i = 0 ; i < 3 ; i + + ) {
for ( int j = 0 ; j < 3 ; j + + ) {
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dots [ j ] + = s [ i ] * abs ( m . get_column ( i ) . normalized ( ) . dot ( b . get_column ( j ) ) ) ;
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}
}
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if ( sign ! = signbit ( dots . x + dots . y + dots . z ) ) {
dots = - dots ;
}
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m . scale_local ( Vector3 ( 1 , 1 , 1 ) + dots ) ;
return m ;
}
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float Basis : : get_uniform_scale ( ) const {
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return ( rows [ 0 ] . length ( ) + rows [ 1 ] . length ( ) + rows [ 2 ] . length ( ) ) / 3.0f ;
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}
Restore the behavior of Spatial rotations recently changed in c1153f5.
That change was borne out of a confusion regarding the meaning of "local" in #14569.
Affine transformations in Spatial simply correspond to affine operations of its Transform. Such operations take place in a coordinate system that is defined by the parent Spatial. When there is no parent, they correspond to operations in the global coordinate system.
This coordinate system, which is relative to the parent, has been referred to as the local coordinate system in the docs so far, but this sloppy language has apparently confused some users, making them think that the local coordinate system refers to the one whose axes are "painted" on the Spatial node itself.
To avoid such conceptual conflations and misunderstandings in the future, the parent-relative local system is now referred to as "parent-local", and the object-relative local system is called "object-local" in the docs.
This commit adds the functionality "requested" in #14569, not by changing how rotate/scale/translate works, but by adding new rotate_object_local, scale_object_local and translate_object_local functions. Also, for completeness, there is now global_scale.
This commit also updates another part of the docs regarding the rotation property of Spatial, which also leads to confusion among some users.
2017-12-27 00:15:20 +00:00
Basis Basis : : scaled_local ( const Vector3 & p_scale ) const {
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return ( * this ) * Basis : : from_scale ( p_scale ) ;
Restore the behavior of Spatial rotations recently changed in c1153f5.
That change was borne out of a confusion regarding the meaning of "local" in #14569.
Affine transformations in Spatial simply correspond to affine operations of its Transform. Such operations take place in a coordinate system that is defined by the parent Spatial. When there is no parent, they correspond to operations in the global coordinate system.
This coordinate system, which is relative to the parent, has been referred to as the local coordinate system in the docs so far, but this sloppy language has apparently confused some users, making them think that the local coordinate system refers to the one whose axes are "painted" on the Spatial node itself.
To avoid such conceptual conflations and misunderstandings in the future, the parent-relative local system is now referred to as "parent-local", and the object-relative local system is called "object-local" in the docs.
This commit adds the functionality "requested" in #14569, not by changing how rotate/scale/translate works, but by adding new rotate_object_local, scale_object_local and translate_object_local functions. Also, for completeness, there is now global_scale.
This commit also updates another part of the docs regarding the rotation property of Spatial, which also leads to confusion among some users.
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}
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Vector3 Basis : : get_scale_abs ( ) const {
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return Vector3 (
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Vector3 ( rows [ 0 ] [ 0 ] , rows [ 1 ] [ 0 ] , rows [ 2 ] [ 0 ] ) . length ( ) ,
Vector3 ( rows [ 0 ] [ 1 ] , rows [ 1 ] [ 1 ] , rows [ 2 ] [ 1 ] ) . length ( ) ,
Vector3 ( rows [ 0 ] [ 2 ] , rows [ 1 ] [ 2 ] , rows [ 2 ] [ 2 ] ) . length ( ) ) ;
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}
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Vector3 Basis : : get_scale_local ( ) const {
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real_t det_sign = SIGN ( determinant ( ) ) ;
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return det_sign * Vector3 ( rows [ 0 ] . length ( ) , rows [ 1 ] . length ( ) , rows [ 2 ] . length ( ) ) ;
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}
// get_scale works with get_rotation, use get_scale_abs if you need to enforce positive signature.
Vector3 Basis : : get_scale ( ) const {
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// FIXME: We are assuming M = R.S (R is rotation and S is scaling), and use polar decomposition to extract R and S.
// A polar decomposition is M = O.P, where O is an orthogonal matrix (meaning rotation and reflection) and
// P is a positive semi-definite matrix (meaning it contains absolute values of scaling along its diagonal).
//
// Despite being different from what we want to achieve, we can nevertheless make use of polar decomposition
// here as follows. We can split O into a rotation and a reflection as O = R.Q, and obtain M = R.S where
// we defined S = Q.P. Now, R is a proper rotation matrix and S is a (signed) scaling matrix,
// which can involve negative scalings. However, there is a catch: unlike the polar decomposition of M = O.P,
// the decomposition of O into a rotation and reflection matrix as O = R.Q is not unique.
// Therefore, we are going to do this decomposition by sticking to a particular convention.
// This may lead to confusion for some users though.
//
// The convention we use here is to absorb the sign flip into the scaling matrix.
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// The same convention is also used in other similar functions such as get_rotation_axis_angle, get_rotation, ...
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//
// A proper way to get rid of this issue would be to store the scaling values (or at least their signs)
// as a part of Basis. However, if we go that path, we need to disable direct (write) access to the
// matrix elements.
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//
// The rotation part of this decomposition is returned by get_rotation* functions.
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real_t det_sign = SIGN ( determinant ( ) ) ;
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return det_sign * get_scale_abs ( ) ;
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}
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// Decomposes a Basis into a rotation-reflection matrix (an element of the group O(3)) and a positive scaling matrix as B = O.S.
// Returns the rotation-reflection matrix via reference argument, and scaling information is returned as a Vector3.
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// This (internal) function is too specific and named too ugly to expose to users, and probably there's no need to do so.
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Vector3 Basis : : rotref_posscale_decomposition ( Basis & rotref ) const {
# ifdef MATH_CHECKS
ERR_FAIL_COND_V ( determinant ( ) = = 0 , Vector3 ( ) ) ;
Basis m = transposed ( ) * ( * this ) ;
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ERR_FAIL_COND_V ( ! m . is_diagonal ( ) , Vector3 ( ) ) ;
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# endif
Vector3 scale = get_scale ( ) ;
Basis inv_scale = Basis ( ) . scaled ( scale . inverse ( ) ) ; // this will also absorb the sign of scale
rotref = ( * this ) * inv_scale ;
# ifdef MATH_CHECKS
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ERR_FAIL_COND_V ( ! rotref . is_orthogonal ( ) , Vector3 ( ) ) ;
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# endif
return scale . abs ( ) ;
}
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// Multiplies the matrix from left by the rotation matrix: M -> R.M
// Note that this does *not* rotate the matrix itself.
//
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// The main use of Basis is as Transform.basis, which is used by the transformation matrix
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// of 3D object. Rotate here refers to rotation of the object (which is R * (*this)),
// not the matrix itself (which is R * (*this) * R.transposed()).
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Basis Basis : : rotated ( const Vector3 & p_axis , real_t p_angle ) const {
return Basis ( p_axis , p_angle ) * ( * this ) ;
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}
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void Basis : : rotate ( const Vector3 & p_axis , real_t p_angle ) {
* this = rotated ( p_axis , p_angle ) ;
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}
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void Basis : : rotate_local ( const Vector3 & p_axis , real_t p_angle ) {
Restore the behavior of Spatial rotations recently changed in c1153f5.
That change was borne out of a confusion regarding the meaning of "local" in #14569.
Affine transformations in Spatial simply correspond to affine operations of its Transform. Such operations take place in a coordinate system that is defined by the parent Spatial. When there is no parent, they correspond to operations in the global coordinate system.
This coordinate system, which is relative to the parent, has been referred to as the local coordinate system in the docs so far, but this sloppy language has apparently confused some users, making them think that the local coordinate system refers to the one whose axes are "painted" on the Spatial node itself.
To avoid such conceptual conflations and misunderstandings in the future, the parent-relative local system is now referred to as "parent-local", and the object-relative local system is called "object-local" in the docs.
This commit adds the functionality "requested" in #14569, not by changing how rotate/scale/translate works, but by adding new rotate_object_local, scale_object_local and translate_object_local functions. Also, for completeness, there is now global_scale.
This commit also updates another part of the docs regarding the rotation property of Spatial, which also leads to confusion among some users.
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// performs a rotation in object-local coordinate system:
// M -> (M.R.Minv).M = M.R.
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* this = rotated_local ( p_axis , p_angle ) ;
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}
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Basis Basis : : rotated_local ( const Vector3 & p_axis , real_t p_angle ) const {
return ( * this ) * Basis ( p_axis , p_angle ) ;
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}
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Basis Basis : : rotated ( const Vector3 & p_euler , EulerOrder p_order ) const {
return Basis : : from_euler ( p_euler , p_order ) * ( * this ) ;
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}
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void Basis : : rotate ( const Vector3 & p_euler , EulerOrder p_order ) {
* this = rotated ( p_euler , p_order ) ;
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}
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Basis Basis : : rotated ( const Quaternion & p_quaternion ) const {
return Basis ( p_quaternion ) * ( * this ) ;
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}
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void Basis : : rotate ( const Quaternion & p_quaternion ) {
* this = rotated ( p_quaternion ) ;
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}
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Vector3 Basis : : get_euler_normalized ( EulerOrder p_order ) const {
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// Assumes that the matrix can be decomposed into a proper rotation and scaling matrix as M = R.S,
// and returns the Euler angles corresponding to the rotation part, complementing get_scale().
// See the comment in get_scale() for further information.
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Basis m = orthonormalized ( ) ;
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real_t det = m . determinant ( ) ;
if ( det < 0 ) {
// Ensure that the determinant is 1, such that result is a proper rotation matrix which can be represented by Euler angles.
m . scale ( Vector3 ( - 1 , - 1 , - 1 ) ) ;
}
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return m . get_euler ( p_order ) ;
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}
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Quaternion Basis : : get_rotation_quaternion ( ) const {
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// Assumes that the matrix can be decomposed into a proper rotation and scaling matrix as M = R.S,
// and returns the Euler angles corresponding to the rotation part, complementing get_scale().
// See the comment in get_scale() for further information.
Basis m = orthonormalized ( ) ;
real_t det = m . determinant ( ) ;
if ( det < 0 ) {
// Ensure that the determinant is 1, such that result is a proper rotation matrix which can be represented by Euler angles.
m . scale ( Vector3 ( - 1 , - 1 , - 1 ) ) ;
}
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return m . get_quaternion ( ) ;
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}
New and improved IK system for Skeleton3D
This PR and commit adds a new IK system for 3D with the Skeleton3D node
that adds several new IK solvers, as well as additional changes and functionality
for making bone manipulation in Godot easier.
This work was sponsored by GSoC 2020 and TwistedTwigleg
Full list of changes:
* Adds a SkeletonModification3D resource
* This resource is the base where all IK code is written and executed
* Adds a SkeletonModificationStack3D resource
* This node oversees the execution of the modifications and acts as a bridge of sorts for the modifications to the Skeleton3D node
* Adds SkeletonModification3D resources for LookAt, CCDIK, FABRIK, Jiggle, and TwoBoneIK
* Each modification is in it's own file
* Several changes to Skeletons, listed below:
* Added local_pose_override, which acts just like global_pose_override but keeps bone-child relationships intract
* So if you move a bone using local_pose_override, all of the bones that are children will also be moved. This is different than global_pose_override, which only affects the individual bone
* Internally bones keep track of their children. This removes the need of a processing list, makes it possible to update just a few select bones at a time, and makes it easier to traverse down the bone chain
* Additional functions added for converting from world transform to global poses, global poses to local poses, and all the same changes but backwards (local to global, global to world). This makes it much easier to work with bone transforms without needing to think too much about how to convert them.
* New signal added, bone_pose_changed, that can be used to tell if a specific bone changed its transform. Needed for BoneAttachment3D
* Added functions for getting the forward position of a bone
* BoneAttachment3D node refactored heavily
* BoneAttachment3D node is now completely standalone in its functionality.
* This makes the code easier and less interconnected, as well as allowing them to function properly without being direct children of Skeleton3D nodes
* BoneAttachment3D now can be set either using the index or the bone name.
* BoneAttachment3D nodes can now set the bone transform instead of just following it. This is disabled by default for compatibility
* BoneAttachment3D now shows a warning when not configured correctly
* Added rotate_to_align function in Basis
* Added class reference documentation for all changes
2020-08-03 21:22:34 +00:00
void Basis : : rotate_to_align ( Vector3 p_start_direction , Vector3 p_end_direction ) {
// Takes two vectors and rotates the basis from the first vector to the second vector.
// Adopted from: https://gist.github.com/kevinmoran/b45980723e53edeb8a5a43c49f134724
const Vector3 axis = p_start_direction . cross ( p_end_direction ) . normalized ( ) ;
if ( axis . length_squared ( ) ! = 0 ) {
real_t dot = p_start_direction . dot ( p_end_direction ) ;
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dot = CLAMP ( dot , - 1.0f , 1.0f ) ;
New and improved IK system for Skeleton3D
This PR and commit adds a new IK system for 3D with the Skeleton3D node
that adds several new IK solvers, as well as additional changes and functionality
for making bone manipulation in Godot easier.
This work was sponsored by GSoC 2020 and TwistedTwigleg
Full list of changes:
* Adds a SkeletonModification3D resource
* This resource is the base where all IK code is written and executed
* Adds a SkeletonModificationStack3D resource
* This node oversees the execution of the modifications and acts as a bridge of sorts for the modifications to the Skeleton3D node
* Adds SkeletonModification3D resources for LookAt, CCDIK, FABRIK, Jiggle, and TwoBoneIK
* Each modification is in it's own file
* Several changes to Skeletons, listed below:
* Added local_pose_override, which acts just like global_pose_override but keeps bone-child relationships intract
* So if you move a bone using local_pose_override, all of the bones that are children will also be moved. This is different than global_pose_override, which only affects the individual bone
* Internally bones keep track of their children. This removes the need of a processing list, makes it possible to update just a few select bones at a time, and makes it easier to traverse down the bone chain
* Additional functions added for converting from world transform to global poses, global poses to local poses, and all the same changes but backwards (local to global, global to world). This makes it much easier to work with bone transforms without needing to think too much about how to convert them.
* New signal added, bone_pose_changed, that can be used to tell if a specific bone changed its transform. Needed for BoneAttachment3D
* Added functions for getting the forward position of a bone
* BoneAttachment3D node refactored heavily
* BoneAttachment3D node is now completely standalone in its functionality.
* This makes the code easier and less interconnected, as well as allowing them to function properly without being direct children of Skeleton3D nodes
* BoneAttachment3D now can be set either using the index or the bone name.
* BoneAttachment3D nodes can now set the bone transform instead of just following it. This is disabled by default for compatibility
* BoneAttachment3D now shows a warning when not configured correctly
* Added rotate_to_align function in Basis
* Added class reference documentation for all changes
2020-08-03 21:22:34 +00:00
const real_t angle_rads = Math : : acos ( dot ) ;
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* this = Basis ( axis , angle_rads ) * ( * this ) ;
New and improved IK system for Skeleton3D
This PR and commit adds a new IK system for 3D with the Skeleton3D node
that adds several new IK solvers, as well as additional changes and functionality
for making bone manipulation in Godot easier.
This work was sponsored by GSoC 2020 and TwistedTwigleg
Full list of changes:
* Adds a SkeletonModification3D resource
* This resource is the base where all IK code is written and executed
* Adds a SkeletonModificationStack3D resource
* This node oversees the execution of the modifications and acts as a bridge of sorts for the modifications to the Skeleton3D node
* Adds SkeletonModification3D resources for LookAt, CCDIK, FABRIK, Jiggle, and TwoBoneIK
* Each modification is in it's own file
* Several changes to Skeletons, listed below:
* Added local_pose_override, which acts just like global_pose_override but keeps bone-child relationships intract
* So if you move a bone using local_pose_override, all of the bones that are children will also be moved. This is different than global_pose_override, which only affects the individual bone
* Internally bones keep track of their children. This removes the need of a processing list, makes it possible to update just a few select bones at a time, and makes it easier to traverse down the bone chain
* Additional functions added for converting from world transform to global poses, global poses to local poses, and all the same changes but backwards (local to global, global to world). This makes it much easier to work with bone transforms without needing to think too much about how to convert them.
* New signal added, bone_pose_changed, that can be used to tell if a specific bone changed its transform. Needed for BoneAttachment3D
* Added functions for getting the forward position of a bone
* BoneAttachment3D node refactored heavily
* BoneAttachment3D node is now completely standalone in its functionality.
* This makes the code easier and less interconnected, as well as allowing them to function properly without being direct children of Skeleton3D nodes
* BoneAttachment3D now can be set either using the index or the bone name.
* BoneAttachment3D nodes can now set the bone transform instead of just following it. This is disabled by default for compatibility
* BoneAttachment3D now shows a warning when not configured correctly
* Added rotate_to_align function in Basis
* Added class reference documentation for all changes
2020-08-03 21:22:34 +00:00
}
}
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void Basis : : get_rotation_axis_angle ( Vector3 & p_axis , real_t & p_angle ) const {
// Assumes that the matrix can be decomposed into a proper rotation and scaling matrix as M = R.S,
// and returns the Euler angles corresponding to the rotation part, complementing get_scale().
// See the comment in get_scale() for further information.
Basis m = orthonormalized ( ) ;
real_t det = m . determinant ( ) ;
if ( det < 0 ) {
// Ensure that the determinant is 1, such that result is a proper rotation matrix which can be represented by Euler angles.
m . scale ( Vector3 ( - 1 , - 1 , - 1 ) ) ;
}
m . get_axis_angle ( p_axis , p_angle ) ;
}
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void Basis : : get_rotation_axis_angle_local ( Vector3 & p_axis , real_t & p_angle ) const {
// Assumes that the matrix can be decomposed into a proper rotation and scaling matrix as M = R.S,
// and returns the Euler angles corresponding to the rotation part, complementing get_scale().
// See the comment in get_scale() for further information.
Basis m = transposed ( ) ;
m . orthonormalize ( ) ;
real_t det = m . determinant ( ) ;
if ( det < 0 ) {
// Ensure that the determinant is 1, such that result is a proper rotation matrix which can be represented by Euler angles.
m . scale ( Vector3 ( - 1 , - 1 , - 1 ) ) ;
}
m . get_axis_angle ( p_axis , p_angle ) ;
p_angle = - p_angle ;
}
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Vector3 Basis : : get_euler ( EulerOrder p_order ) const {
switch ( p_order ) {
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case EulerOrder : : XYZ : {
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// Euler angles in XYZ convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cy*cz -cy*sz sy
// cz*sx*sy+cx*sz cx*cz-sx*sy*sz -cy*sx
// -cx*cz*sy+sx*sz cz*sx+cx*sy*sz cx*cy
Vector3 euler ;
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real_t sy = rows [ 0 ] [ 2 ] ;
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if ( sy < ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
if ( sy > - ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
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// is this a pure Y rotation?
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if ( rows [ 1 ] [ 0 ] = = 0 & & rows [ 0 ] [ 1 ] = = 0 & & rows [ 1 ] [ 2 ] = = 0 & & rows [ 2 ] [ 1 ] = = 0 & & rows [ 1 ] [ 1 ] = = 1 ) {
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// return the simplest form (human friendlier in editor and scripts)
euler . x = 0 ;
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euler . y = atan2 ( rows [ 0 ] [ 2 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = 0 ;
} else {
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euler . x = Math : : atan2 ( - rows [ 1 ] [ 2 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = Math : : asin ( sy ) ;
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euler . z = Math : : atan2 ( - rows [ 0 ] [ 1 ] , rows [ 0 ] [ 0 ] ) ;
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}
} else {
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
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euler . y = - Math_PI / 2.0f ;
euler . z = 0.0f ;
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}
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} else {
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
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euler . y = Math_PI / 2.0f ;
euler . z = 0.0f ;
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}
return euler ;
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}
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case EulerOrder : : XZY : {
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// Euler angles in XZY convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cz*cy -sz cz*sy
// sx*sy+cx*cy*sz cx*cz cx*sz*sy-cy*sx
// cy*sx*sz cz*sx cx*cy+sx*sz*sy
Vector3 euler ;
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real_t sz = rows [ 0 ] [ 1 ] ;
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if ( sz < ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
if ( sz > - ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
euler . y = Math : : atan2 ( rows [ 0 ] [ 2 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = Math : : asin ( - sz ) ;
} else {
// It's -1
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euler . x = - Math : : atan2 ( rows [ 1 ] [ 2 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = 0.0f ;
euler . z = Math_PI / 2.0f ;
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}
} else {
// It's 1
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euler . x = - Math : : atan2 ( rows [ 1 ] [ 2 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = 0.0f ;
euler . z = - Math_PI / 2.0f ;
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}
return euler ;
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}
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case EulerOrder : : YXZ : {
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// Euler angles in YXZ convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cy*cz+sy*sx*sz cz*sy*sx-cy*sz cx*sy
// cx*sz cx*cz -sx
// cy*sx*sz-cz*sy cy*cz*sx+sy*sz cy*cx
Vector3 euler ;
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real_t m12 = rows [ 1 ] [ 2 ] ;
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if ( m12 < ( 1 - ( real_t ) CMP_EPSILON ) ) {
if ( m12 > - ( 1 - ( real_t ) CMP_EPSILON ) ) {
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// is this a pure X rotation?
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if ( rows [ 1 ] [ 0 ] = = 0 & & rows [ 0 ] [ 1 ] = = 0 & & rows [ 0 ] [ 2 ] = = 0 & & rows [ 2 ] [ 0 ] = = 0 & & rows [ 0 ] [ 0 ] = = 1 ) {
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// return the simplest form (human friendlier in editor and scripts)
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euler . x = atan2 ( - m12 , rows [ 1 ] [ 1 ] ) ;
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euler . y = 0 ;
euler . z = 0 ;
} else {
euler . x = asin ( - m12 ) ;
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euler . y = atan2 ( rows [ 0 ] [ 2 ] , rows [ 2 ] [ 2 ] ) ;
euler . z = atan2 ( rows [ 1 ] [ 0 ] , rows [ 1 ] [ 1 ] ) ;
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}
} else { // m12 == -1
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euler . x = Math_PI * 0.5f ;
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euler . y = atan2 ( rows [ 0 ] [ 1 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = 0 ;
}
} else { // m12 == 1
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euler . x = - Math_PI * 0.5f ;
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euler . y = - atan2 ( rows [ 0 ] [ 1 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = 0 ;
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}
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return euler ;
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}
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case EulerOrder : : YZX : {
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// Euler angles in YZX convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cy*cz sy*sx-cy*cx*sz cx*sy+cy*sz*sx
// sz cz*cx -cz*sx
// -cz*sy cy*sx+cx*sy*sz cy*cx-sy*sz*sx
Vector3 euler ;
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real_t sz = rows [ 1 ] [ 0 ] ;
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if ( sz < ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
if ( sz > - ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
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euler . x = Math : : atan2 ( - rows [ 1 ] [ 2 ] , rows [ 1 ] [ 1 ] ) ;
euler . y = Math : : atan2 ( - rows [ 2 ] [ 0 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = Math : : asin ( sz ) ;
} else {
// It's -1
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = 0.0f ;
euler . z = - Math_PI / 2.0f ;
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}
} else {
// It's 1
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = 0.0f ;
euler . z = Math_PI / 2.0f ;
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}
return euler ;
} break ;
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case EulerOrder : : ZXY : {
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// Euler angles in ZXY convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cz*cy-sz*sx*sy -cx*sz cz*sy+cy*sz*sx
// cy*sz+cz*sx*sy cz*cx sz*sy-cz*cy*sx
// -cx*sy sx cx*cy
Vector3 euler ;
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real_t sx = rows [ 2 ] [ 1 ] ;
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if ( sx < ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
if ( sx > - ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
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euler . x = Math : : asin ( sx ) ;
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euler . y = Math : : atan2 ( - rows [ 2 ] [ 0 ] , rows [ 2 ] [ 2 ] ) ;
euler . z = Math : : atan2 ( - rows [ 0 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
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} else {
// It's -1
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euler . x = - Math_PI / 2.0f ;
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euler . y = Math : : atan2 ( rows [ 0 ] [ 2 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = 0 ;
}
} else {
// It's 1
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euler . x = Math_PI / 2.0f ;
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euler . y = Math : : atan2 ( rows [ 0 ] [ 2 ] , rows [ 0 ] [ 0 ] ) ;
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euler . z = 0 ;
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}
return euler ;
} break ;
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case EulerOrder : : ZYX : {
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// Euler angles in ZYX convention.
// See https://en.wikipedia.org/wiki/Euler_angles#Rotation_matrix
//
// rot = cz*cy cz*sy*sx-cx*sz sz*sx+cz*cx*cy
// cy*sz cz*cx+sz*sy*sx cx*sz*sy-cz*sx
// -sy cy*sx cy*cx
Vector3 euler ;
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real_t sy = rows [ 2 ] [ 0 ] ;
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if ( sy < ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
if ( sy > - ( 1.0f - ( real_t ) CMP_EPSILON ) ) {
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euler . x = Math : : atan2 ( rows [ 2 ] [ 1 ] , rows [ 2 ] [ 2 ] ) ;
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euler . y = Math : : asin ( - sy ) ;
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euler . z = Math : : atan2 ( rows [ 1 ] [ 0 ] , rows [ 0 ] [ 0 ] ) ;
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} else {
// It's -1
euler . x = 0 ;
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euler . y = Math_PI / 2.0f ;
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euler . z = - Math : : atan2 ( rows [ 0 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
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}
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} else {
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// It's 1
euler . x = 0 ;
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euler . y = - Math_PI / 2.0f ;
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euler . z = - Math : : atan2 ( rows [ 0 ] [ 1 ] , rows [ 1 ] [ 1 ] ) ;
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}
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return euler ;
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}
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default : {
ERR_FAIL_V_MSG ( Vector3 ( ) , " Invalid parameter for get_euler(order) " ) ;
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}
}
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return Vector3 ( ) ;
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}
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void Basis : : set_euler ( const Vector3 & p_euler , EulerOrder p_order ) {
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real_t c , s ;
c = Math : : cos ( p_euler . x ) ;
s = Math : : sin ( p_euler . x ) ;
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Basis xmat ( 1 , 0 , 0 , 0 , c , - s , 0 , s , c ) ;
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c = Math : : cos ( p_euler . y ) ;
s = Math : : sin ( p_euler . y ) ;
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Basis ymat ( c , 0 , s , 0 , 1 , 0 , - s , 0 , c ) ;
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c = Math : : cos ( p_euler . z ) ;
s = Math : : sin ( p_euler . z ) ;
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Basis zmat ( c , - s , 0 , s , c , 0 , 0 , 0 , 1 ) ;
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switch ( p_order ) {
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case EulerOrder : : XYZ : {
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* this = xmat * ( ymat * zmat ) ;
} break ;
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case EulerOrder : : XZY : {
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* this = xmat * zmat * ymat ;
} break ;
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case EulerOrder : : YXZ : {
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* this = ymat * xmat * zmat ;
} break ;
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case EulerOrder : : YZX : {
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* this = ymat * zmat * xmat ;
} break ;
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case EulerOrder : : ZXY : {
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* this = zmat * xmat * ymat ;
} break ;
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case EulerOrder : : ZYX : {
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* this = zmat * ymat * xmat ;
} break ;
default : {
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ERR_FAIL_MSG ( " Invalid Euler order parameter. " ) ;
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}
}
}
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bool Basis : : is_equal_approx ( const Basis & p_basis ) const {
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return rows [ 0 ] . is_equal_approx ( p_basis . rows [ 0 ] ) & & rows [ 1 ] . is_equal_approx ( p_basis . rows [ 1 ] ) & & rows [ 2 ] . is_equal_approx ( p_basis . rows [ 2 ] ) ;
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}
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bool Basis : : is_finite ( ) const {
return rows [ 0 ] . is_finite ( ) & & rows [ 1 ] . is_finite ( ) & & rows [ 2 ] . is_finite ( ) ;
}
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bool Basis : : operator = = ( const Basis & p_matrix ) const {
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for ( int i = 0 ; i < 3 ; i + + ) {
for ( int j = 0 ; j < 3 ; j + + ) {
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if ( rows [ i ] [ j ] ! = p_matrix . rows [ i ] [ j ] ) {
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return false ;
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}
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}
}
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return true ;
}
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bool Basis : : operator ! = ( const Basis & p_matrix ) const {
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return ( ! ( * this = = p_matrix ) ) ;
}
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Basis : : operator String ( ) const {
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return " [X: " + get_column ( 0 ) . operator String ( ) +
" , Y: " + get_column ( 1 ) . operator String ( ) +
" , Z: " + get_column ( 2 ) . operator String ( ) + " ] " ;
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}
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Quaternion Basis : : get_quaternion ( ) const {
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# ifdef MATH_CHECKS
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ERR_FAIL_COND_V_MSG ( ! is_rotation ( ) , Quaternion ( ) , " Basis " + operator String ( ) + " must be normalized in order to be casted to a Quaternion. Use get_rotation_quaternion() or call orthonormalized() if the Basis contains linearly independent vectors. " ) ;
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# endif
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/* Allow getting a quaternion from an unnormalized transform */
Basis m = * this ;
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real_t trace = m . rows [ 0 ] [ 0 ] + m . rows [ 1 ] [ 1 ] + m . rows [ 2 ] [ 2 ] ;
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real_t temp [ 4 ] ;
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if ( trace > 0.0f ) {
real_t s = Math : : sqrt ( trace + 1.0f ) ;
temp [ 3 ] = ( s * 0.5f ) ;
s = 0.5f / s ;
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temp [ 0 ] = ( ( m . rows [ 2 ] [ 1 ] - m . rows [ 1 ] [ 2 ] ) * s ) ;
temp [ 1 ] = ( ( m . rows [ 0 ] [ 2 ] - m . rows [ 2 ] [ 0 ] ) * s ) ;
temp [ 2 ] = ( ( m . rows [ 1 ] [ 0 ] - m . rows [ 0 ] [ 1 ] ) * s ) ;
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} else {
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int i = m . rows [ 0 ] [ 0 ] < m . rows [ 1 ] [ 1 ]
? ( m . rows [ 1 ] [ 1 ] < m . rows [ 2 ] [ 2 ] ? 2 : 1 )
: ( m . rows [ 0 ] [ 0 ] < m . rows [ 2 ] [ 2 ] ? 2 : 0 ) ;
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int j = ( i + 1 ) % 3 ;
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int k = ( i + 2 ) % 3 ;
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real_t s = Math : : sqrt ( m . rows [ i ] [ i ] - m . rows [ j ] [ j ] - m . rows [ k ] [ k ] + 1.0f ) ;
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temp [ i ] = s * 0.5f ;
s = 0.5f / s ;
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temp [ 3 ] = ( m . rows [ k ] [ j ] - m . rows [ j ] [ k ] ) * s ;
temp [ j ] = ( m . rows [ j ] [ i ] + m . rows [ i ] [ j ] ) * s ;
temp [ k ] = ( m . rows [ k ] [ i ] + m . rows [ i ] [ k ] ) * s ;
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}
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return Quaternion ( temp [ 0 ] , temp [ 1 ] , temp [ 2 ] , temp [ 3 ] ) ;
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}
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void Basis : : get_axis_angle ( Vector3 & r_axis , real_t & r_angle ) const {
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/* checking this is a bad idea, because obtaining from scaled transform is a valid use case
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# ifdef MATH_CHECKS
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ERR_FAIL_COND ( ! is_rotation ( ) ) ;
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# endif
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*/
// https://www.euclideanspace.com/maths/geometry/rotations/conversions/matrixToAngle/index.htm
real_t x , y , z ; // Variables for result.
if ( Math : : is_zero_approx ( rows [ 0 ] [ 1 ] - rows [ 1 ] [ 0 ] ) & & Math : : is_zero_approx ( rows [ 0 ] [ 2 ] - rows [ 2 ] [ 0 ] ) & & Math : : is_zero_approx ( rows [ 1 ] [ 2 ] - rows [ 2 ] [ 1 ] ) ) {
// Singularity found.
// First check for identity matrix which must have +1 for all terms in leading diagonal and zero in other terms.
if ( is_diagonal ( ) & & ( Math : : abs ( rows [ 0 ] [ 0 ] + rows [ 1 ] [ 1 ] + rows [ 2 ] [ 2 ] - 3 ) < 3 * CMP_EPSILON ) ) {
// This singularity is identity matrix so angle = 0.
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r_axis = Vector3 ( 0 , 1 , 0 ) ;
r_angle = 0 ;
return ;
}
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// Otherwise this singularity is angle = 180.
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real_t xx = ( rows [ 0 ] [ 0 ] + 1 ) / 2 ;
real_t yy = ( rows [ 1 ] [ 1 ] + 1 ) / 2 ;
real_t zz = ( rows [ 2 ] [ 2 ] + 1 ) / 2 ;
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real_t xy = ( rows [ 0 ] [ 1 ] + rows [ 1 ] [ 0 ] ) / 4 ;
real_t xz = ( rows [ 0 ] [ 2 ] + rows [ 2 ] [ 0 ] ) / 4 ;
real_t yz = ( rows [ 1 ] [ 2 ] + rows [ 2 ] [ 1 ] ) / 4 ;
if ( ( xx > yy ) & & ( xx > zz ) ) { // rows[0][0] is the largest diagonal term.
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if ( xx < CMP_EPSILON ) {
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x = 0 ;
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y = Math_SQRT12 ;
z = Math_SQRT12 ;
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} else {
x = Math : : sqrt ( xx ) ;
y = xy / x ;
z = xz / x ;
}
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} else if ( yy > zz ) { // rows[1][1] is the largest diagonal term.
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if ( yy < CMP_EPSILON ) {
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x = Math_SQRT12 ;
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y = 0 ;
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z = Math_SQRT12 ;
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} else {
y = Math : : sqrt ( yy ) ;
x = xy / y ;
z = yz / y ;
}
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} else { // rows[2][2] is the largest diagonal term so base result on this.
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if ( zz < CMP_EPSILON ) {
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x = Math_SQRT12 ;
y = Math_SQRT12 ;
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z = 0 ;
} else {
z = Math : : sqrt ( zz ) ;
x = xz / z ;
y = yz / z ;
}
}
r_axis = Vector3 ( x , y , z ) ;
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r_angle = Math_PI ;
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return ;
}
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// As we have reached here there are no singularities so we can handle normally.
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double s = Math : : sqrt ( ( rows [ 2 ] [ 1 ] - rows [ 1 ] [ 2 ] ) * ( rows [ 2 ] [ 1 ] - rows [ 1 ] [ 2 ] ) + ( rows [ 0 ] [ 2 ] - rows [ 2 ] [ 0 ] ) * ( rows [ 0 ] [ 2 ] - rows [ 2 ] [ 0 ] ) + ( rows [ 1 ] [ 0 ] - rows [ 0 ] [ 1 ] ) * ( rows [ 1 ] [ 0 ] - rows [ 0 ] [ 1 ] ) ) ; // Used to normalize.
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if ( Math : : abs ( s ) < CMP_EPSILON ) {
// Prevent divide by zero, should not happen if matrix is orthogonal and should be caught by singularity test above.
s = 1 ;
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}
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x = ( rows [ 2 ] [ 1 ] - rows [ 1 ] [ 2 ] ) / s ;
y = ( rows [ 0 ] [ 2 ] - rows [ 2 ] [ 0 ] ) / s ;
z = ( rows [ 1 ] [ 0 ] - rows [ 0 ] [ 1 ] ) / s ;
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r_axis = Vector3 ( x , y , z ) ;
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// acos does clamping.
r_angle = Math : : acos ( ( rows [ 0 ] [ 0 ] + rows [ 1 ] [ 1 ] + rows [ 2 ] [ 2 ] - 1 ) / 2 ) ;
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}
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void Basis : : set_quaternion ( const Quaternion & p_quaternion ) {
real_t d = p_quaternion . length_squared ( ) ;
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real_t s = 2.0f / d ;
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real_t xs = p_quaternion . x * s , ys = p_quaternion . y * s , zs = p_quaternion . z * s ;
real_t wx = p_quaternion . w * xs , wy = p_quaternion . w * ys , wz = p_quaternion . w * zs ;
real_t xx = p_quaternion . x * xs , xy = p_quaternion . x * ys , xz = p_quaternion . x * zs ;
real_t yy = p_quaternion . y * ys , yz = p_quaternion . y * zs , zz = p_quaternion . z * zs ;
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set ( 1.0f - ( yy + zz ) , xy - wz , xz + wy ,
xy + wz , 1.0f - ( xx + zz ) , yz - wx ,
xz - wy , yz + wx , 1.0f - ( xx + yy ) ) ;
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}
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void Basis : : set_axis_angle ( const Vector3 & p_axis , real_t p_angle ) {
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// Rotation matrix from axis and angle, see https://en.wikipedia.org/wiki/Rotation_matrix#Rotation_matrix_from_axis_angle
# ifdef MATH_CHECKS
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ERR_FAIL_COND_MSG ( ! p_axis . is_normalized ( ) , " The axis Vector3 " + p_axis . operator String ( ) + " must be normalized. " ) ;
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# endif
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Vector3 axis_sq ( p_axis . x * p_axis . x , p_axis . y * p_axis . y , p_axis . z * p_axis . z ) ;
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real_t cosine = Math : : cos ( p_angle ) ;
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rows [ 0 ] [ 0 ] = axis_sq . x + cosine * ( 1.0f - axis_sq . x ) ;
rows [ 1 ] [ 1 ] = axis_sq . y + cosine * ( 1.0f - axis_sq . y ) ;
rows [ 2 ] [ 2 ] = axis_sq . z + cosine * ( 1.0f - axis_sq . z ) ;
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real_t sine = Math : : sin ( p_angle ) ;
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real_t t = 1 - cosine ;
real_t xyzt = p_axis . x * p_axis . y * t ;
real_t zyxs = p_axis . z * sine ;
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rows [ 0 ] [ 1 ] = xyzt - zyxs ;
rows [ 1 ] [ 0 ] = xyzt + zyxs ;
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xyzt = p_axis . x * p_axis . z * t ;
zyxs = p_axis . y * sine ;
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rows [ 0 ] [ 2 ] = xyzt + zyxs ;
rows [ 2 ] [ 0 ] = xyzt - zyxs ;
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xyzt = p_axis . y * p_axis . z * t ;
zyxs = p_axis . x * sine ;
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rows [ 1 ] [ 2 ] = xyzt - zyxs ;
rows [ 2 ] [ 1 ] = xyzt + zyxs ;
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}
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void Basis : : set_axis_angle_scale ( const Vector3 & p_axis , real_t p_angle , const Vector3 & p_scale ) {
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_set_diagonal ( p_scale ) ;
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rotate ( p_axis , p_angle ) ;
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}
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void Basis : : set_euler_scale ( const Vector3 & p_euler , const Vector3 & p_scale , EulerOrder p_order ) {
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_set_diagonal ( p_scale ) ;
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rotate ( p_euler , p_order ) ;
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}
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void Basis : : set_quaternion_scale ( const Quaternion & p_quaternion , const Vector3 & p_scale ) {
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_set_diagonal ( p_scale ) ;
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rotate ( p_quaternion ) ;
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}
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// This also sets the non-diagonal elements to 0, which is misleading from the
// name, so we want this method to be private. Use `from_scale` externally.
void Basis : : _set_diagonal ( const Vector3 & p_diag ) {
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rows [ 0 ] [ 0 ] = p_diag . x ;
rows [ 0 ] [ 1 ] = 0 ;
rows [ 0 ] [ 2 ] = 0 ;
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rows [ 1 ] [ 0 ] = 0 ;
rows [ 1 ] [ 1 ] = p_diag . y ;
rows [ 1 ] [ 2 ] = 0 ;
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rows [ 2 ] [ 0 ] = 0 ;
rows [ 2 ] [ 1 ] = 0 ;
rows [ 2 ] [ 2 ] = p_diag . z ;
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}
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Basis Basis : : lerp ( const Basis & p_to , const real_t & p_weight ) const {
Basis b ;
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b . rows [ 0 ] = rows [ 0 ] . lerp ( p_to . rows [ 0 ] , p_weight ) ;
b . rows [ 1 ] = rows [ 1 ] . lerp ( p_to . rows [ 1 ] , p_weight ) ;
b . rows [ 2 ] = rows [ 2 ] . lerp ( p_to . rows [ 2 ] , p_weight ) ;
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return b ;
}
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Basis Basis : : slerp ( const Basis & p_to , const real_t & p_weight ) const {
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//consider scale
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Quaternion from ( * this ) ;
Quaternion to ( p_to ) ;
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Basis b ( from . slerp ( to , p_weight ) ) ;
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b . rows [ 0 ] * = Math : : lerp ( rows [ 0 ] . length ( ) , p_to . rows [ 0 ] . length ( ) , p_weight ) ;
b . rows [ 1 ] * = Math : : lerp ( rows [ 1 ] . length ( ) , p_to . rows [ 1 ] . length ( ) , p_weight ) ;
b . rows [ 2 ] * = Math : : lerp ( rows [ 2 ] . length ( ) , p_to . rows [ 2 ] . length ( ) , p_weight ) ;
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return b ;
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}
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void Basis : : rotate_sh ( real_t * p_values ) {
// code by John Hable
// http://filmicworlds.com/blog/simple-and-fast-spherical-harmonic-rotation/
// this code is Public Domain
const static real_t s_c3 = 0.94617469575 ; // (3*sqrt(5))/(4*sqrt(pi))
const static real_t s_c4 = - 0.31539156525 ; // (-sqrt(5))/(4*sqrt(pi))
const static real_t s_c5 = 0.54627421529 ; // (sqrt(15))/(4*sqrt(pi))
const static real_t s_c_scale = 1.0 / 0.91529123286551084 ;
const static real_t s_c_scale_inv = 0.91529123286551084 ;
const static real_t s_rc2 = 1.5853309190550713 * s_c_scale ;
const static real_t s_c4_div_c3 = s_c4 / s_c3 ;
const static real_t s_c4_div_c3_x2 = ( s_c4 / s_c3 ) * 2.0 ;
const static real_t s_scale_dst2 = s_c3 * s_c_scale_inv ;
const static real_t s_scale_dst4 = s_c5 * s_c_scale_inv ;
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const real_t src [ 9 ] = { p_values [ 0 ] , p_values [ 1 ] , p_values [ 2 ] , p_values [ 3 ] , p_values [ 4 ] , p_values [ 5 ] , p_values [ 6 ] , p_values [ 7 ] , p_values [ 8 ] } ;
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real_t m00 = rows [ 0 ] [ 0 ] ;
real_t m01 = rows [ 0 ] [ 1 ] ;
real_t m02 = rows [ 0 ] [ 2 ] ;
real_t m10 = rows [ 1 ] [ 0 ] ;
real_t m11 = rows [ 1 ] [ 1 ] ;
real_t m12 = rows [ 1 ] [ 2 ] ;
real_t m20 = rows [ 2 ] [ 0 ] ;
real_t m21 = rows [ 2 ] [ 1 ] ;
real_t m22 = rows [ 2 ] [ 2 ] ;
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p_values [ 0 ] = src [ 0 ] ;
p_values [ 1 ] = m11 * src [ 1 ] - m12 * src [ 2 ] + m10 * src [ 3 ] ;
p_values [ 2 ] = - m21 * src [ 1 ] + m22 * src [ 2 ] - m20 * src [ 3 ] ;
p_values [ 3 ] = m01 * src [ 1 ] - m02 * src [ 2 ] + m00 * src [ 3 ] ;
real_t sh0 = src [ 7 ] + src [ 8 ] + src [ 8 ] - src [ 5 ] ;
real_t sh1 = src [ 4 ] + s_rc2 * src [ 6 ] + src [ 7 ] + src [ 8 ] ;
real_t sh2 = src [ 4 ] ;
real_t sh3 = - src [ 7 ] ;
real_t sh4 = - src [ 5 ] ;
// Rotations. R0 and R1 just use the raw matrix columns
real_t r2x = m00 + m01 ;
real_t r2y = m10 + m11 ;
real_t r2z = m20 + m21 ;
real_t r3x = m00 + m02 ;
real_t r3y = m10 + m12 ;
real_t r3z = m20 + m22 ;
real_t r4x = m01 + m02 ;
real_t r4y = m11 + m12 ;
real_t r4z = m21 + m22 ;
// dense matrix multiplication one column at a time
// column 0
real_t sh0_x = sh0 * m00 ;
real_t sh0_y = sh0 * m10 ;
real_t d0 = sh0_x * m10 ;
real_t d1 = sh0_y * m20 ;
real_t d2 = sh0 * ( m20 * m20 + s_c4_div_c3 ) ;
real_t d3 = sh0_x * m20 ;
real_t d4 = sh0_x * m00 - sh0_y * m10 ;
// column 1
real_t sh1_x = sh1 * m02 ;
real_t sh1_y = sh1 * m12 ;
d0 + = sh1_x * m12 ;
d1 + = sh1_y * m22 ;
d2 + = sh1 * ( m22 * m22 + s_c4_div_c3 ) ;
d3 + = sh1_x * m22 ;
d4 + = sh1_x * m02 - sh1_y * m12 ;
// column 2
real_t sh2_x = sh2 * r2x ;
real_t sh2_y = sh2 * r2y ;
d0 + = sh2_x * r2y ;
d1 + = sh2_y * r2z ;
d2 + = sh2 * ( r2z * r2z + s_c4_div_c3_x2 ) ;
d3 + = sh2_x * r2z ;
d4 + = sh2_x * r2x - sh2_y * r2y ;
// column 3
real_t sh3_x = sh3 * r3x ;
real_t sh3_y = sh3 * r3y ;
d0 + = sh3_x * r3y ;
d1 + = sh3_y * r3z ;
d2 + = sh3 * ( r3z * r3z + s_c4_div_c3_x2 ) ;
d3 + = sh3_x * r3z ;
d4 + = sh3_x * r3x - sh3_y * r3y ;
// column 4
real_t sh4_x = sh4 * r4x ;
real_t sh4_y = sh4 * r4y ;
d0 + = sh4_x * r4y ;
d1 + = sh4_y * r4z ;
d2 + = sh4 * ( r4z * r4z + s_c4_div_c3_x2 ) ;
d3 + = sh4_x * r4z ;
d4 + = sh4_x * r4x - sh4_y * r4y ;
// extra multipliers
p_values [ 4 ] = d0 ;
p_values [ 5 ] = - d1 ;
p_values [ 6 ] = d2 * s_scale_dst2 ;
p_values [ 7 ] = - d3 ;
p_values [ 8 ] = d4 * s_scale_dst4 ;
}
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Basis Basis : : looking_at ( const Vector3 & p_target , const Vector3 & p_up , bool p_use_model_front ) {
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# ifdef MATH_CHECKS
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ERR_FAIL_COND_V_MSG ( p_target . is_zero_approx ( ) , Basis ( ) , " The target vector can't be zero. " ) ;
ERR_FAIL_COND_V_MSG ( p_up . is_zero_approx ( ) , Basis ( ) , " The up vector can't be zero. " ) ;
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# endif
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Vector3 v_z = p_target . normalized ( ) ;
if ( ! p_use_model_front ) {
v_z = - v_z ;
}
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Vector3 v_x = p_up . cross ( v_z ) ;
# ifdef MATH_CHECKS
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ERR_FAIL_COND_V_MSG ( v_x . is_zero_approx ( ) , Basis ( ) , " The target vector and up vector can't be parallel to each other. " ) ;
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# endif
v_x . normalize ( ) ;
Vector3 v_y = v_z . cross ( v_x ) ;
Basis basis ;
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basis . set_columns ( v_x , v_y , v_z ) ;
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return basis ;
}